Determining a size of cell of a transmission spectroscopy device

ABSTRACT

A transmission spectroscopy device can direct light into a sample, and determine properties of the sample based on how much light emerges from the sample. The device can use a cell to contain the sample, so that the size of the cell defines the optical path length traversed by light in the sample. To ensure accuracy in the measurements, it is beneficial to calibrate the device by measuring the size of the cell periodically or as needed. To measure the size of the cell, the device can perform a transmission spectroscopy measurement of a known substance, such as pure water, to produce a measured absorbance spectrum of the known substance. The device can subtract a known absorbance spectrum of the known substance from the measured absorbance spectrum to form an oscillatory fringe pattern. The device can determine the size of the cell from a period of the fringe pattern.

PRIORITY APPLICATION

This application is a divisional of, and claims priority to U.S. patentapplication Ser. No. 15/292,593, filed Oct. 13, 2016, the disclosure ofwhich is incorporated herein in its entirety by reference.

FIELD OF THE DISCLOSURE

The present disclosure relates to calibration of a transmissionspectroscopy device.

BACKGROUND OF THE DISCLOSURE

Transmission spectroscopy is widely used for quantitatively measuringcomponents of gaseous, liquid and solid substances. A transmissionspectroscopy device can direct light into a sample, and determineproperties of the sample based on how much light emerges from thesample, as a function of wavelength.

In some examples, a transmission spectroscopy device can base itscalculations on the Beer-Lambert law, which relates the attenuation oflight to properties of the material through which the light propagates.One way to express the Beer-Lambert law mathematically is A=e×b×c.Quantity A is the absorbance of the sample, which also equals log(1/transmittance of the sample). Quantity e is the molar absorptivity ofa compound of interest in the sample. Quantity b is the optical pathlength traversed by light in the sample. Quantity c is the concentrationof the compound of interest in the sample. In order to produce anaccurate value for the compound concentration, c, one should have anaccurate value for the optical path length traversed by light in thesample, b. The Beer-Lambert law is but one example of how a transmissionspectroscopy device can perform its calculations. Other calculationtechniques can also be used. For each of these calculation techniques,it is beneficial to know or measure the optical path length traversed bylight in the sample as accurately as possible.

SUMMARY

In a first example, a method for determining a size of a cell of atransmission spectroscopy device can include performing a transmissionspectroscopy measurement of a known substance in a cell to produce ameasured absorbance spectrum of the known substance. The measuredabsorbance spectrum of the known substance can be formed from a ratio ofa first emittance scan of the cell to a second emittance scan of thecell. The first emittance scan can be taken when the cell is filled withthe known substance. The second emittance scan can be taken when thecell is empty. The method can further include subtracting a knownabsorbance spectrum of the known substance from the measured absorbancespectrum of the known substance to form a fringe pattern. The fringepattern can be oscillatory in amplitude with respect to inversewavelength. The method can further include determining a size of thecell from a period of the fringe pattern.

In a second example, a transmission spectroscopy device can include acell having opposing first and second transparent walls. The cell can befillable with a sample to be measured. The cell can be drainable toremove the sample and replace the sample with air. Plumbing can deliverthe sample to the cell and drain the sample from the cell. A lightsource can illuminate the sample through the first transparent wall. Adetector can detect light transmitted through the sample through thesecond transparent wall. A controller can operably control the lightsource, operably receive at least one signal from the detector, andoperably control the plumbing. The controller can fill the cell with thesample, produce a measured absorbance spectrum of the sample, and drainthe sample from the cell. The controller can further calibrate thetransmission spectroscopy device by: producing a measured absorbancespectrum of a pure water sample, the measured absorbance spectrum of thepure water sample formed from a ratio of a first emittance scan of thecell to a second emittance scan of the cell, the first emittance scantaken when the cell is filled with the pure water sample, the secondemittance scan taken when the cell is empty; subtracting a knownabsorbance spectrum of water from the measured absorbance spectrum ofthe pure water sample to form a fringe pattern, the fringe pattern beingoscillatory in amplitude with respect to inverse wavelength; andcalculating the separation between the first and second transparentwalls to equal 1/(2×p), where quantity p is a period of the fringepattern.

In a third example, a method for determining a size of cell of atransmission spectroscopy device can include performing a transmissionspectroscopy measurement of a pure water sample in a cell to produce ameasured absorbance spectrum of the pure water sample. The measuredabsorbance spectrum of the pure water sample can be formed from a ratioof a first emittance scan of the cell to a second emittance scan of thecell. The first emittance scan can be taken when the cell is filled withthe pure water sample. The second emittance scan can be taken when thecell is empty. The method can further include subtracting a knownabsorbance spectrum of water from the measured absorbance spectrum ofthe pure water sample to form a fringe pattern. The fringe pattern canbe oscillatory in amplitude with respect to inverse wavelength. Themethod can further include calculating a separation between opposingfirst and second transparent walls of the cell to equal 1/(2×p), wherequantity p is a period of the fringe pattern.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows a schematic drawing of an example of a transmissionspectroscopy device, in accordance with some embodiments.

FIG. 2 shows a flowchart of an example of a method for determining asize of a cell of a transmission spectroscopy device, in accordance withsome embodiments.

FIG. 3 shows an example of a plot of measured absorbance spectrum ofwater, a known absorbance spectrum of water, and a fringe pattern, inaccordance with some embodiments.

FIG. 4 shows an example of a plot of the inverse wavelength values atwhich the fringe pattern of FIG. 3 peaks, plotted along a linear scaleby dimensionless peak number.

FIG. 5 shows a relative fat error, in percent, for measurements in whichthe cell width was periodically measured, and corresponding measurementsin which the cell width was not periodically measured or updated.

FIG. 6 shows a relative protein error, in percent, for measurements inwhich the cell width was periodically measured, and correspondingmeasurements in which the cell width was not periodically measured orupdated.

FIG. 7 shows a relative solids error, in percent, for measurements inwhich the cell width was periodically measured, and correspondingmeasurements in which the cell width was not periodically measured orupdated.

Corresponding reference characters indicate corresponding partsthroughout the several views. Elements in the drawings are notnecessarily drawn to scale. The configurations shown in the drawings aremerely examples, and should not be construed as necessarily limiting thescope of the claims.

DETAILED DESCRIPTION

In transmission spectroscopy, it is beneficial to know or measure theoptical path length traversed by light in the sample as accurately aspossible. For gaseous or liquid samples, a transmission spectroscopydevice can use a cell or cuvette to contain the sample. The cell caninclude two opposing, transparent walls. During a measurement, lightenters the cell through one of the transparent walls, passes through thesample, and exits the cell through the other of the transparent walls.The size of the cell defines the optical path length traversed by lightin the sample. In some examples, the size of the cell can refer to acell width, a cell length, or another suitable cell dimension. To ensureaccuracy in the measurements, it is beneficial to calibrate thetransmission spectroscopy device by measuring the size of the cellperiodically or as needed.

To measure the size of the cell, the device can perform a transmissionspectroscopy measurement of a known substance, such as pure water, toproduce a measured absorbance spectrum of the known substance. Thedevice can subtract a known absorbance spectrum of the known substancefrom the measured absorbance spectrum to form an oscillatory fringepattern. The fringes can be Fabry-Perot fringes, caused by interferencefrom reflections from two parallel surfaces. The fringes can be presentin the measured absorption spectrum, but masked by larger absorbanceeffects. Subtracting the known absorbance spectrum from the measuredabsorbance spectrum can remove or reduce the absorbance effects, and canemphasize the fringe pattern in the measured absorption spectrum. Thedevice can determine the size of the cell from a period of the fringepattern. This is but a summary of a technique to measure the size of thecell; the technique is discussed below in more detail, following adescription of a transmission spectroscopy device.

FIG. 1 shows a schematic drawing of an example of a transmissionspectroscopy device 100, in accordance with some embodiments. Thetransmission spectroscopy device 100 is but one example of a device thatcan use the technique described herein to measure the size of the cell;other devices can also be used.

A cell 102 can have a first transparent wall 104 and a secondtransparent wall 106 opposing the first transparent wall 104. The cell102 can be fillable with a sample to be measured. The sample is not partof the part of the transmission spectroscopy device 100. The cell can bedrainable to remove the sample and replace the sample with air. In someexamples, the first transparent wall 104 and the second transparent wall106 can be formed from glass, calcium fluoride, or other suitablematerials selected to be insoluble with respect to the sample. In someexamples, the first transparent wall 104 and the second transparent wall106 can have a nominal separation between 10 μm and 50 μm.

In some examples, the separation between the first transparent wall 104and the second transparent wall 106 can vary slightly over time. Forexample, the separation can increase slightly if the first transparentwall 104 and the second transparent wall 106 are eroded by continualuse. Likewise, the separation can decrease slightly if samples cause abuildup of material on the first transparent wall 104 and the secondtransparent wall 106. The technique described herein to measure the sizeof the cell 102 can track the cell size variation over time, and canallow the transmission spectroscopy device 100 to properly account forcell size and perform accurate measurements. The cell size measurementtechnique can be used as a calibration routine, which can be executedperiodically, such as once a day, or once for every thousandmeasurements.

Plumbing 108 can deliver the sample to the cell 102 and can drain thesample from the cell 102. The plumbing 108 can include one or morepipes, hoses, valves, pumps, and other elements can direct fluids orgases as needed. The plumbing 108 can include one or more connections tothe cell 102. In some examples, the plumbing 108 can direct the sampleinto or out of the transmission spectroscopy device 100, and can connectto one or more elements outside the transmission spectroscopy device100. In some examples, the plumbing 108 can deliver air to the cell 102.In some examples, the plumbing 108 can pump air to the cell 102, todrain the cell of a sample.

A light source 110 can illuminate the sample through the firsttransparent wall 104. In some examples, the light source 110 can be abroadband light source, such as a blackbody source, an incandescentsource, one or more light emitting diodes, or other suitable lightsources. In some examples, the light source 110 produces a collimatedoutput beam. In some examples, the light source 110 includes one or morecollimating lenses, which can collimate light from a diverging source,such as a light emitting diode, to produce a collimated output beam. Insome examples, the light source 110 can emit light in the mid-infraredportion of the spectrum. In some examples, the light source 110 can emitlight with wavelengths between 1.25 μm and 12.5 μm, or, equivalently,inverse wavelengths between 800 cm⁻¹ (corresponding to 12.5 μm) and 8000cm⁻¹ (corresponding to 1.25 μm). Other wavelength ranges can also beused, including the visible portion of the spectrum, the near-infraredportion of the spectrum, or the far infrared portion of the spectrum.

A detector 112 can detect light transmitted through the sample throughthe second transparent wall 106. In some examples, the detector 112 issensitive in the wavelength range emitted by the light source 110.

A controller 114 can operably control the light source 110, operablyreceive at least one signal from the detector 112, and operably controlthe plumbing 108. During execution of the cell size measurementtechnique, the controller 114 can fill the cell 102 with the sample,produce a measured absorbance spectrum of the sample, and drain thesample from the cell 102. In some examples, the controller 114 caninclude a processor and memory, including instructions that, whenexecuted on the at least processor, cause the processor to execute thetechnique to measure the size of the cell.

The transmission spectroscopy device 100 can further include aspectrometer 116 that can receive light emitted from the light source110, and can analyze the received light as a function of wavelength. Insome examples, the spectrometer 116 can include a diffraction grating, aprism, or another optical element capable of spatially or angularlydispersing light as a function of wavelength. In some examples, in aconfiguration referred to as dispersive spectroscopy, the spectrometer116 has a selectable output wavelength (or narrow band of wavelengths),which can be controlled by the controller 114, and can vary over time.The controller 114 can correlate the wavelength output of thespectrometer, over time, with the signal received at the detector 112,to measure a sample in the cell 102 as a function of wavelength. Inother examples, the spectrometer can analyze the wavelength dependenceof the transmitted light signal by generating an interferogram producedby the varying the optical path length of two interfering light beams.The Fourier transform of this interferogram results in a spectrum ofintensity vs. wavelength (or energy, often in units of 1/wavelength).This technique is referred to as Fourier Transform Spectroscopy, and hasseveral advantages over dispersive spectroscopy in terms of opticalthroughput and wavelength multiplexing. Positioning the spectrometer 116between the light source 110 and the cell 102 is but one configuration.Other configurations can also be used, such as positioning thespectrometer 116 between the cell 102 and the detector 112, using amulti-element detector to simultaneously capture light at differentwavelengths for the dispersive technique, and others. The spectrometer116 can receive and output collimated light.

The transmission spectroscopy device 100 can further include a lens 118that can focus light from the spectrometer 116 onto the cell 102, and alens 120 that can focus light from the cell onto the detector 112. Thelens 118 can allow the transmission spectroscopy device 100 to use arelatively small cell 102, which can advantageously take measurements ofsamples having a relatively small volume. The lens 120 can allow thetransmission spectroscopy device 100 to use a relatively small detector112, which can advantageously reduce noise associated with the detector112 and can increase the speed of the detector 112.

The transmission spectroscopy device 100 can further include a housing122, which can ensure that the cell 102 operates in an environment thatis stable over time. For example, the housing 122 can control thetemperature and pressure of the sample in the cell 102. The housing 122can maintain a constant composition of the gases, such as water vaporand carbon dioxide, around the cell 102 and the optical elements. Thehousing 122 can be sealed from the ambient environment. The housing 122can be temperature-regulated. The housing 122 can include a desiccant toreduce water vapor to a relatively low and stable level. Stabilizing theenvironmental variables of temperature, pressure and the composition ofthe gases in the optical path can increase a precision of themeasurements. Stabilizing these parameters can stabilize the opticalalignment of the spectrometer, which can increase the precision of themeasurements.

FIG. 2 shows a flowchart of an example of a method 200 for determining asize of a cell of a transmission spectroscopy device 100, in accordancewith some embodiments. The method 200 can be executed on a transmissionspectroscopy device, such as device 100 (described above with referenceto FIG. 1), or on other suitable transmission spectroscopy devices. Themethod 200 is but one example of determining the size of the cell; othersuitable methods can also be used.

At operation 202, the device 100 can perform a transmission spectroscopymeasurement of a known substance in a cell 102 to produce a measuredabsorbance spectrum of the known substance. The measured absorbancespectrum of the known substance can be formed from a ratio of a firstemittance scan of the cell 102 to a second emittance scan of the cell102. The first emittance scan can be taken when the cell 102 is filledwith the known substance. The second emittance scan can be taken whenthe cell 102 is empty (e.g., filled with air).

At operation 204, the device 100 can subtract a known absorbancespectrum of the known substance from the measured absorbance spectrum ofthe known substance to form a fringe pattern. In some examples, theknown absorbance spectrum can be stored locally and can be access via alookup table. In other examples, the known absorbance spectrum can beaccessed remotely through a wired or wireless network. In some examples,the known absorbance spectrum can be obtained from an earliertransmission spectroscopy measurement of a particular sample (e.g., notnecessarily a sample having a tabulated absorbance spectrum).

The fringe pattern can be caused by interference between opposing firstand second transparent walls 104, 106 of the cell 102. The fringepattern peaks when there is constructive interference between the firstand second transparent walls 104, 106 of the cell 102, which occurs whenthe round-trip optical path between the first and second transparentwalls 104, 106 equals an integral number of wavelengths. In general, thefringe pattern is smaller in amplitude than the features in the measuredabsorbance spectrum, so that subtracting the known absorbance spectrumof the known substance from the measured absorbance spectrum can enhancethe fringe pattern. The fringe pattern can be oscillatory in amplitudewith respect to inverse wavelength. In some examples, the device 100 canscale an amplitude of one of the known absorbance spectrum or themeasured absorbance spectrum to match an amplitude of the other of theknown absorbance spectrum or the measured absorbance spectrum.

At operation 206, the device 100 can determine a size of the cell 102from a period of the fringe pattern. In some examples, the device 100can calculate a separation between opposing first and second transparentwalls 104, 106 of the cell 102 to equal 1/(2×p), where quantity p is aperiod of the fringe pattern. In some examples, the device 100 candetermine inverse wavelength values at which the fringe pattern peaks,and calculate the period to equal a separation between adjacentdetermined inverse wavelength values. In some examples, the device 100can fit the determined inverse wavelength values to a linear fit,determine a slope of the linear fit, and set the period equal to thedetermined slope.

In some examples, performing the transmission spectroscopy measurementof the known substance in the cell 102 can include the following. Thedevice 100 can fill the cell 102 with the known substance. The device100 can illuminate the known substance through a first transparent wall104 of the cell 102. In some example, the illuminating light has a broadspectrum. The device 100 can measure a first light from the knownsubstance through a second transparent wall 106 of the cell 102,opposite the first transparent wall 104. The device 100 can produce,from the first light, the first emittance scan. The device 100 can drainthe known substance from the cell 102. The device 100 can fill the cell102 with air. The device 100 can illuminate the air-filled cell 102through the first transparent wall 104 of the cell 102. In some example,the illuminating light for the air-filled cell can have the same broadspectrum as the illuminating light used for the known substance. Thedevice 100 can measure a second light from the air-filled cell 102through the second transparent wall 106 of the cell 102. The device 100can produce, from the second light, the second emittance scan. In someconfigurations, the device 100 can measure the sample before measuringthe air-filled cell; in other configurations, the device 100 can measurethe sample after measuring the air-filled cell.

In some examples, draining the known substance from the cell 102 caninclude, repeatedly: pumping air through the cell 102; illuminating thecell 102 through the first transparent wall 104 of the cell 102;measuring a third light through the second transparent wall 106 of thecell 102; and comparing the third light to a previous measurement of thethird light, until a difference between successive measurements of thethird light is below a threshold. As the cell 102 dries out, the amountof light passing through the cell reaches a constant level.

In some examples, the known substance can be pure water, although otherknown substances can also be used. For these examples, the broadspectrum of the illuminating light can include at least one peak orvalley in the known absorbance spectrum of water. For example, in thenear-infrared and mid-infrared wavelength ranges, liquid water hasabsorption bands around 1640 cm⁻¹ (corresponding to a wavelength of 6100nm), 2130 cm⁻¹ (4690 nm), 3450 cm⁻¹ (2900 nm), and 5128 cm⁻¹ (1950 nm).It is convenient to use values of inverse wavelength, rather thanwavelength, because the fringes in the fringe pattern are equally spacedwith respect to inverse wavelength.

FIG. 3 shows an example of a plot of a measured absorbance spectrum 302of water, a known absorbance spectrum 304 of water, and a fringe pattern306, in accordance with some embodiments. The measured absorbancespectrum 302 and the known absorbance spectrum 304 overlapsignificantly; the element numbers 302 and 304 follow the respectiveplots in FIG. 3. In practice, the fringe pattern 306 is present in themeasured absorbance spectrum 302, but with a significantly smalleramplitude than the absorption features. Subtracting the known absorbancespectrum 304 from the measured absorbance spectrum 302 of water(optionally with scaling of one or both absorbance spectra) can enhancethe fringe pattern 306. In this example, the fringe pattern extends fromabout 3900 cm⁻¹ to about 6900 cm⁻¹, with a discontinuity in the fringepattern around water's absorption band at 5128 cm⁻¹.

The period of the fringe pattern can be determined in many suitablemanners, including Fourier transforming the fringe pattern and locatinga peak in the Fourier transform, finding peaks in the fringe anddetermining separation between the peaks, finding valleys in the fringepattern and determining separation between the valleys, findingzero-crossings in the fringe patterns and determining separation betweenthe zero-crossings, and others.

One suitable way to calculate the period includes: determining inversewavelength values at which the fringe pattern peaks; fitting thedetermined inverse wavelength values to a linear fit; determining aslope of the linear fit; and setting the period equal to the determinedslope.

FIG. 4 shows an example of a plot of the inverse wavelength values atwhich the fringe pattern of FIG. 3 peaks, plotted along a linear scaleby dimensionless peak number. The inverse wavelength values are fit to alinear fit, according to the equation: y [in cm⁻¹]=148.43x+2142.8. Theslope of the linear fit is 148.43 cm⁻¹, which equals the period of thefringe pattern. In this numerical example, the separation betweenopposing first and second transparent walls 104, 106 of the cell 102equals 1/(2×148.43 cm⁻¹), or 33.69 μm. This is but one example; othersuitable numerical examples can also be used.

It is beneficial to consider a set of experimental data that shows theeffectiveness of periodically measuring the size of the cell, as withthe method 200. Data was taken for a milk inspection system over thecourse of seven months. In this example, the milk inspection systeminspected raw milk samples using the mid-infrared portion of thespectrum (e.g., with wavelengths between 3 μm and 10 μm). The systemused chemometric calibration methods to relate the measured milkspectrum to a component concentration, for components, such as fat,protein, and solids. The system operated in a relatively demandingenvironment, running more than 4000 samples per day, with relativelyhigh accuracy, and relatively high potential for cell wear from the highsample volume. The system measured the samples with an accuracy relativestandard deviation of less than 1% and a repeatability relative standarddeviation of less than 0.25%. In this example, the inspection systemtested a set of thirteen reference milk standards over a course of sevenmonths. FIG. 5 shows a relative fat error, in percent, for measurementsin which the cell width was periodically measured (502), andcorresponding measurements in which the cell width was not periodicallymeasured or updated (504). FIG. 6 shows a relative protein error, inpercent, for measurements in which the cell width was periodicallymeasured (602), and corresponding measurements in which the cell widthwas not periodically measured or updated (604). FIG. 7 shows a relativesolids error, in percent, for measurements in which the cell width wasperiodically measured (702), and corresponding measurements in which thecell width was not periodically measured or updated (704). In each ofFIGS. 5-7, the relative error grew with time when the cell width was notperiodically measured or updated, but remained relatively small andrelatively constant over time when the cell width was periodicallymeasured and updated.

The method 200 for determining the size of the cell 102 of thetransmission spectroscopy device 100 has significant advantages overother approaches for determining the size.

For example, a first approach of determining a cell size takes ameasurement of a sample of a precisely known composition, measures itsabsorption at particular wavelengths, and determines the optical pathlength traversed in the sample from the Beer-Lambert law and from atabulated molar absorptivity of the compound. This first approach issubject to errors caused by producing, maintaining and deliveringsamples of precisely known composition. The method 200 discussed hereinis not subject to producing, maintaining and delivering samples ofprecisely known composition, as is required in the first approach.

As another example, a second approach of determining a cell size removesthe cell from the device, measures the cell size externally using aninterferometer or other suitable measurement device, then returns thecell to the device for future use. This second approach istime-consuming and disruptive, especially for devices that operate in atightly controlled environment with regulated temperature, pressure, andhumidity. The time lost for cell size measurements can be especiallyproblematic for high-volume applications. The method 200 discussedherein can be performed in situ, with a relatively short times requiredfor the measurement.

While the embodiments above have been described as having exampledesigns, inventive aspects of these embodiments can be further modifiedwithin the spirit and scope of this disclosure. This application istherefore intended to cover any variations, uses, or adaptations of theembodiments using their general principles. Further, this application isintended to cover such departures from the present disclosure as comewithin known or customary practice in the art to which this subjectmatter pertains and which fall within the limits of the appended claims.

What is claimed is:
 1. A transmission spectroscopy device, comprising: a cell having opposing first and second transparent walls, the cell being fillable with a sample to be measured, the cell being drainable to remove the sample and replace the sample with air; and a controller configured to fill the cell with the sample, produce a measured absorbance spectrum of the sample, and drain the sample from the cell, the controller further configured to calibrate the transmission spectroscopy device by: producing a measured absorbance spectrum of a known substance sample of a known substance, the measured absorbance spectrum of the known substance sample formed from a ratio of a first emittance scan of the cell to a second emittance scan of the cell, the first emittance scan taken when the cell is filled with the known substance sample, the second emittance scan taken when the cell is empty; subtracting a known absorbance spectrum of the known substance from the measured absorbance spectrum of the known substance sample to form a fringe pattern, the fringe pattern being oscillatory in amplitude with respect to inverse wavelength; and determining a size of the cell from a period of the fringe pattern.
 2. The transmission spectroscopy device of claim 1, wherein the controller is further configured to determine the size of the cell from the period of the fringe pattern by: calculating the separation between the first and second transparent walls to equal 1/(2×p), where quantity p is a period of the fringe pattern.
 3. The transmission spectroscopy device of claim 2, wherein the controller is further configured to determine the size of the cell from the period of the fringe pattern by: determining inverse wavelength values at which the fringe pattern peaks; and calculating the period to equal a separation between adjacent determined inverse wavelength values.
 4. The transmission spectroscopy device of claim 3, wherein the controller is further configured to calculate the period by: fitting the determined inverse wavelength values to a linear fit; determining a slope of the linear fit; and setting the period equal to the determined slope.
 5. The transmission spectroscopy device of claim 1, wherein the controller is further configured to produce the measured absorbance spectrum of the known substance sample of the known substance by: filling the cell with the known substance; illuminating the known substance through the first transparent wall of the cell; measuring a first light from the known substance through the second transparent wall of the cell; producing, from the first light, the first emittance scan; draining the known substance from the cell; filling the cell with air; illuminating the air-filled cell through the first transparent wall of the cell; measuring a second light from the air-filled cell through the second transparent wall of the cell; and producing, from the second light, the second emittance scan.
 6. The transmission spectroscopy device of claim 5, wherein the size of the cell corresponds to a separation between the first and second transparent walls of the cell.
 7. The transmission spectroscopy device of claim 5, further comprising: a light source configured to provide illumination to the known substance and the air-filled cell through the first transparent wall with light having a broad spectrum, the controller being further configured to operably control the light source.
 8. The transmission spectroscopy device of claim 7, wherein: the known substance is water; and the broad spectrum includes at least one peak or valley in the known absorbance spectrum of water.
 9. The transmission spectroscopy device of claim 5, wherein the controller is further configured to drain the known substance from the cell by, repeatedly: pumping air through the cell; illuminating the cell through the first transparent wall of the cell; measuring a third light through the second transparent wall of the cell; and comparing the third light to a previous measurement of the third light, until a difference between successive measurements of the third light is below a threshold.
 10. The transmission spectroscopy device of claim 1, wherein the controller is further configured to subtract the known absorbance spectrum of the known substance from the measured absorbance spectrum by: scaling an amplitude of one of the known absorbance spectrum or the measured absorbance spectrum to match an amplitude of the other of the known absorbance spectrum or the measured absorbance spectrum.
 11. The transmission spectroscopy device of claim 1, further comprising: plumbing configured to deliver the sample to the cell, drain the sample from the cell, deliver the known substance sample to the cell, and drain the known substance sample from the cell, the controller being further configured to operably control the plumbing.
 12. The transmission spectroscopy device of claim 1, further comprising: a detector configured to detect light transmitted through the sample and through the known substance sample through the second transparent wall, the controller further configured to operably receive at least one signal from the detector.
 13. A transmission spectroscopy device, comprising: a cell having opposing first and second transparent walls, the cell being fillable with a sample to be measured, the cell being drainable to remove the sample and replace the sample with air; plumbing configured to deliver the sample to the cell and drain the sample from the cell; a light source configured to illuminate the sample through the first transparent wall; a detector configured to detect light transmitted through the sample through the second transparent wall; and a controller configured to operably control the light source, operably receive at least one signal from the detector, and operably control the plumbing, the controller configured to fill the cell with the sample, produce a measured absorbance spectrum of the sample, and drain the sample from the cell, the controller further configured to calibrate the transmission spectroscopy device by: producing a measured absorbance spectrum of a known substance sample of a known substance, the measured absorbance spectrum of the known substance sample formed from a ratio of a first emittance scan of the cell to a second emittance scan of the cell, the first emittance scan taken when the cell is filled with the known substance sample, the second emittance scan taken when the cell is empty; subtracting a known absorbance spectrum of the known substance from the measured absorbance spectrum of the known substance sample to form a fringe pattern; and determining a size of the cell from the fringe pattern.
 14. The transmission spectroscopy device of claim 13, wherein: the fringe pattern is oscillatory in amplitude with respect to inverse wavelength; and the controller is further configured to determine the size of the cell from the fringe pattern by: calculating the separation between the first and second transparent walls to equal 1/(2×p), where quantity p is a period of the fringe pattern.
 15. The transmission spectroscopy device of claim 14, wherein the controller is further configured to determine the size of the cell from the period of the fringe pattern by: determining inverse wavelength values at which the fringe pattern peaks; and calculating the period to equal a separation between adjacent determined inverse wavelength values.
 16. The transmission spectroscopy device of claim 15, wherein the controller is further configured to calculate the period by: fitting the determined inverse wavelength values to a linear fit; determining a slope of the linear fit; and setting the period equal to the determined slope.
 17. The transmission spectroscopy device of claim 13, wherein the controller is further configured to produce the measured absorbance spectrum of the known substance sample of the known substance by: filling the cell with the known substance; illuminating the known substance through the first transparent wall of the cell; measuring a first light from the known substance through the second transparent wall of the cell; producing, from the first light, the first emittance scan; draining the known substance from the cell; filling the cell with air; illuminating the air-filled cell through the first transparent wall of the cell; measuring a second light from the air-filled cell through the second transparent wall of the cell; and producing, from the second light, the second emittance scan.
 18. The transmission spectroscopy device of claim 17, wherein the size of the cell corresponds to a separation between the first and second transparent walls of the cell.
 19. The transmission spectroscopy device of claim 18, wherein: the known substance is water; and the broad spectrum includes at least one peak or valley in the known absorbance spectrum of water.
 20. A transmission spectroscopy device, comprising: a cell having opposing first and second transparent walls, the cell being fillable with a sample to be measured, the cell being drainable to remove the sample and replace the sample with air; plumbing configured to deliver the sample to the cell and drain the sample from the cell; a light source configured to illuminate the sample through the first transparent wall; a detector configured to detect light transmitted through the sample through the second transparent wall; and a controller configured to operably control the light source, operably receive at least one signal from the detector, and operably control the plumbing, the controller configured to fill the cell with the sample, produce a measured absorbance spectrum of the sample, and drain the sample from the cell, the controller further configured to calibrate the transmission spectroscopy device by: producing a measured absorbance spectrum of a pure water sample, the measured absorbance spectrum of the pure water sample formed from a ratio of a first emittance scan of the cell to a second emittance scan of the cell, the first emittance scan taken when the cell is filled with the pure water sample, the second emittance scan taken when the cell is empty; subtracting a known absorbance spectrum of water from the measured absorbance spectrum of the pure water sample to form a fringe pattern, the fringe pattern being oscillatory in amplitude with respect to inverse wavelength; and calculating the separation between the first and second transparent walls to equal 1/(2×p), where quantity p is a period of the fringe pattern. 